* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Internal Resistance
Mercury-arc valve wikipedia , lookup
Power engineering wikipedia , lookup
Power inverter wikipedia , lookup
Pulse-width modulation wikipedia , lookup
Stepper motor wikipedia , lookup
History of electric power transmission wikipedia , lookup
Electrical substation wikipedia , lookup
Variable-frequency drive wikipedia , lookup
Three-phase electric power wikipedia , lookup
Shockley–Queisser limit wikipedia , lookup
Power MOSFET wikipedia , lookup
Opto-isolator wikipedia , lookup
Electric battery wikipedia , lookup
Rechargeable battery wikipedia , lookup
Voltage regulator wikipedia , lookup
Resistive opto-isolator wikipedia , lookup
Switched-mode power supply wikipedia , lookup
Surge protector wikipedia , lookup
Electrical ballast wikipedia , lookup
Stray voltage wikipedia , lookup
Distribution management system wikipedia , lookup
Voltage optimisation wikipedia , lookup
Current source wikipedia , lookup
Buck converter wikipedia , lookup
Internal Resistance Batteries and Cells Cells and batteries come in all shapes and sizes. They all have their ‘voltage’ marked on the side. This is called the e.m.f. ( E ) of the battery or cell. e.m.f. stands for electromotive force. If a voltmeter is connected to the terminals of a cell, it will measure the e.m.f. V e.m.f. = 1.5 V The e.m.f. tells you how many joules of energy the battery will supply to every coulomb of charge which passes through it. 1 volt is 1 joule per coulomb Internal Resistance Unfortunately, cells and batteries ( and all other voltage supplies ) also have INTERNAL RESISTANCE. It is a nuisance. We use the symbol r to denote internal resistance and it is often drawn as a small resistor inside the voltage supply. V e.m.f. = 1.5 V E r The problem with internal resistance is that it causes the voltage supplied by the supply to drop when you start to use it to supply anything with current. Lost Volts We call this drop in the voltage of the cell the LOST VOLTS. Remember that it only occurs when a current starts to flow. V 1.5 V E r load resistor A Lost Volts We call this drop in the voltage of the cell the LOST VOLTS. Remember that it only occurs when a current starts to flow. V When the switch is closed …. 1.5 V E r …the current starts to flow … load resistor A 0.2 A Lost Volts We call this drop in the voltage of the cell the LOST VOLTS. Remember that it only occurs when a current starts to flow. V t.p.d. = 1.2 V E When the switch is closed …. r …the current starts to flow … …and the battery voltage drops. load resistor A 0.2 A The voltmeter reading is no longer the e.m.f. It is now called the t.p.d. This stands for terminal potential difference. The lost volts = 0.3 V The Terminal Potential Difference This is not always the same. It depends on the size of the lost volts which, in turn, depends on the current in the circuit. 1.2 V E r R 0.2 A 1.2 V The voltage across the load resistor ( R ) will also be equal to the t.p.d. The Equations E = t.p.d. + lost volts Ohm’s law (V = I x R) can be applied in three ways. For the whole circuit E = I x RT For the Internal Resistance lost volts = I x r For the Load Resistor t.p.d. = I x R